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R.M.K COLLEGE OF ENGINEERING AND
TECHNOLOGY
DEPARTMENT OF ECE
EC8252-ELECTRONIC DEVICES
SECOND SEMESTER-I YEAR- (2020-2024 BATCH)
Mrs.P.Sivalakshmi AP/ECE
SESSION:11
DATE: 3.05.2021
2017- Regulation syllabus
Lecture Overview on BJT
• What is a Transistor?
• History
• Types
• Characteristics
• Applications
What is a Transistor?
• Semiconductors: ability to change from
conductor to insulator
• Can either allow current or prohibit current to
flow
• Useful as a switch, but also as an amplifier
• Essential part of many technological advances
A Brief History
• Guglielmo Marconi invents radio in 1895
• Problem: For long distance travel, signal must be amplified
• Lee De Forest improves on Fleming’s original vacuum tube to
amplify signals
• Made use of third electrode
• Too bulky for most applications
The Transistor is Born
• Bell Labs (1947): Bardeen,
Brattain, and Shockley
• Originally made of germanium
• Current transistors made of
doped silicon
How Transistors Work
• Doping: adding small amounts of other
elements to create additional protons or
electrons
• P-Type: dopants lack a fourth valence electron
(Boron, Aluminum)
• N-Type: dopants have an additional (5th)
valence electron (Phosphorus, Arsenic)
• Importance: Current only flows from P to N
Diodes and Bias
• Diode: simple P-N junction.
• Forward Bias: allows current to
flow from P to N.
• Reverse Bias: no current allowed
to flow from N to P.
• Breakdown Voltage: sufficient N
to P voltage of a Zener Diode will
allow for current to flow in this
direction.
The Invention
 Important Features (compared to Vacuum tubes):
- three terminal solid-state device - requires less power
- smaller and lightweight - lower operating voltage
- has rugged construction - more efficient
- no heater requirement
The First Transistor: On Dec 23, 1947, three scientists led by Dr. William Shockley at the
Bell Telephone Laboratories demonstrated the amplifying action of the first transistor.
(Courtesy Bell Telephone Laboratories.)
Co-inventors:
Dr. William Shockley
(seated);
Dr. John Bardeen (left);
Dr. Walter H. Brattain.
Honored with
Nobel Prize in
Physics in 1956
Bipolar Junction transistor
Holes and electrons
determine device characteristics
Three terminal device
Control of two terminal currents
Amplification and switching through 3rd contact
The term transistor was coined by John R. Pierce as a contraction of
the term trans resistance.
The Structure
 Bipolar: both electrons and holes are involved in current flow.
 Junction: has two p-n junctions.
 Transistor: Transfer + Resistor.
 It can be either n-p-n type or p-n-p type.
 Has three regions with three terminals labeled as
i. Emitter (E)
ii. Base (B) and
iii. Collector (C)
The Bipolar Junction Transistor (BJT)
The Structure: npn & pnp
 Base is made much narrow.
 Emitter is heavily doped (p+, n+).
 Base is lightly doped (p-, n-).
 Collector is lightly doped (p, n).
The Structure: npn & pnp
 Transistors can be constructed as two diodes that are
connected together.
Circuit Symbol
 The arrow indicates the direction
of current flow.
 The current flows from collector
to emitter in an n-p-n transistor.
 The arrow is drawn on the
emitter.
 The arrow always points towards
the n-type. So the emitter is n-type
and the transistor is n-p-n type.
Layout and Circuit Symbol: n-p-n Transistor
Circuit Symbol
 The arrow indicates the direction
of current flow.
 The current flows from emitter to
collector in an p-n-p transistor.
 The arrow points towards the n-
type.
 So the base is n-type and
transistor is p-n-p type.
Layout and Circuit Symbol: p-n-p Transistor
Modes of Operation
 Based on the bias voltages applied at the two p-n
junctions, transistors can operate in three modes:
1. Cut-off (both EB and CB junctions are reversed
biased)
2. Saturation (both EB and CB junctions are
forward biased)
3. Active mode (EBJ is forward biased and CBJ is
reversed biased)
 Cut-off and Saturation modes are used in switching
operation.
 Active mode is used in amplification purposes.
Modes of Operation
npn bipolar junction transistor
pnp bipolar junction transistor
Modes of Operation
 Both the junctions are
reversed biased.
 No current can flow through
either of the junctions.
 So the circuit is open.
Cut-off
VBC
+
+
-
-
VBE
Ideal model of BJT
in cut-off.
Modes of Operation
 Both the junctions are
forward biased.
 So the equivalent circuit can
be represented by short-circuit
between the base, emitter and
collector.
Saturation: Ideal Model
VBC
+
+
-
-
VBE
Ideal model of BJT
in saturation.
Active Mode Operation
EBJ:
Forward Biased
CBJ:
Reverse Biased
◦ Forward bias of EBJ injects electrons from emitter into base (Emitter current).
◦ Most electrons shoot through the base into the collector (Collector current).
◦ Some emitted electrons recombine with holes in p-type base (Base Current)
+
+
+
+
+
+
+
+
+
+
-
-
-
-
-
-
-
-
-
-
N P N
E
B
C
electron
Hole
Active Mode Operation
+
+
+
+
+
+
-
-
-
-
-
-
N P N
E C
B
VBE VCB
E-Field
Electron diffusion
Hole diffusion
Active Mode Operation
+
+
+
+
+
+
-
-
-
-
-
-
N P N
E-Field
E C
B
VBE VCB
Electron hole recombination
Active Mode Operation
Collector current
T
BE
V
v
s
C e
I
i 
• The equation above shows that the BJT is indeed a
voltage-dependent current source; thus it can be
used as an amplifier.
Electrons that diffuse across the base to the CBJ junction are swept
across the CBJ depletion to the collector because of the higher potential
applied to the collector
Active Mode Operation
Biasing for Active Mode
Carriers injected from forward bias junction (from the emitter labeled E)
travel through the intermediate layer (BASE, labeled B) and swept into the
COLLECTOR, labeled C by the reverse biased voltage.
EBJ: Forward Biased
CBJ: Reverse Biased
Conceptual Biasing Circuits
npn Transistor
Conceptual Biasing Circuits
pnp Transistor
DC Output Characteristics
IC vs VCE Characteristics of an npn Transistor
Active Breakdown
Saturation 
31
Active
Breakdown
Saturation 
Cutoff
DC Output
Characteristics
IC vs VCE Characteristics of an npn Transistor
Bipolar Junction Transistors: Basics
+
- +
-
IE
IB
IC
IE = IB + IC ………(KCL)
VEC = VEB + VBC ……… (KVL)
Current Gain:
– α is the fraction of electrons that diffuse across the narrow
Base region
– 1- α is the fraction of electrons that recombine with holes in
the Base region to create base current
• The current Gain is expressed in terms of the β (beta) of
the transistor (often called hfe by manufacturers).
• β (beta) is Temperature and Voltage dependent.
• It can vary a lot among transistors (common values for
signal BJT: (20 - 200).
BJT characteristics











1
)
1
(
B
C
E
B
E
C
I
I
I
I
I
I
Active Mode: Terminal Currents
Current Relationships and Amplification
C
E
B
B
C
E
E
C
E
C
I
I
I
I
I
I
I
I
I
I






/
.















B
C
B
B
C
I
I
I
I
I
and
1
1
 As  is close to unity,  is very large, typically around 100.
  represents the current amplification factor from base to
collector.
 The base current is amplified by a factor of  in the collector
circuit in the Active mode.
  is called the Forward Current Gain, often written as  F.
C
C
C
B
I
I
I
I







1
Operation
Region
IB or VCE
Char.
BC and BE
Junctions
Mode
Cutoff IB = Very
small
Reverse &
Reverse
Open
Switch
Saturation VCE = Small Forward &
Forward
Closed
Switch
Active
Linear
VCE =
Moderate
Reverse &
Forward
Linear
Amplifier
Break-
down
VCE =
Large
Beyond
Limits
Overload
Operation region summary
BJT configurations
GAIN CONFIG
How transistor works:
https://www.youtube.com/watch?v=7ukD
KVHnac4

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Introduction to bjt npn &pnp

  • 1.
  • 2.
  • 3. R.M.K COLLEGE OF ENGINEERING AND TECHNOLOGY DEPARTMENT OF ECE EC8252-ELECTRONIC DEVICES SECOND SEMESTER-I YEAR- (2020-2024 BATCH) Mrs.P.Sivalakshmi AP/ECE SESSION:11 DATE: 3.05.2021
  • 5. Lecture Overview on BJT • What is a Transistor? • History • Types • Characteristics • Applications
  • 6. What is a Transistor? • Semiconductors: ability to change from conductor to insulator • Can either allow current or prohibit current to flow • Useful as a switch, but also as an amplifier • Essential part of many technological advances
  • 7. A Brief History • Guglielmo Marconi invents radio in 1895 • Problem: For long distance travel, signal must be amplified • Lee De Forest improves on Fleming’s original vacuum tube to amplify signals • Made use of third electrode • Too bulky for most applications
  • 8. The Transistor is Born • Bell Labs (1947): Bardeen, Brattain, and Shockley • Originally made of germanium • Current transistors made of doped silicon
  • 9. How Transistors Work • Doping: adding small amounts of other elements to create additional protons or electrons • P-Type: dopants lack a fourth valence electron (Boron, Aluminum) • N-Type: dopants have an additional (5th) valence electron (Phosphorus, Arsenic) • Importance: Current only flows from P to N
  • 10. Diodes and Bias • Diode: simple P-N junction. • Forward Bias: allows current to flow from P to N. • Reverse Bias: no current allowed to flow from N to P. • Breakdown Voltage: sufficient N to P voltage of a Zener Diode will allow for current to flow in this direction.
  • 11. The Invention  Important Features (compared to Vacuum tubes): - three terminal solid-state device - requires less power - smaller and lightweight - lower operating voltage - has rugged construction - more efficient - no heater requirement The First Transistor: On Dec 23, 1947, three scientists led by Dr. William Shockley at the Bell Telephone Laboratories demonstrated the amplifying action of the first transistor. (Courtesy Bell Telephone Laboratories.) Co-inventors: Dr. William Shockley (seated); Dr. John Bardeen (left); Dr. Walter H. Brattain. Honored with Nobel Prize in Physics in 1956
  • 12. Bipolar Junction transistor Holes and electrons determine device characteristics Three terminal device Control of two terminal currents Amplification and switching through 3rd contact The term transistor was coined by John R. Pierce as a contraction of the term trans resistance.
  • 13. The Structure  Bipolar: both electrons and holes are involved in current flow.  Junction: has two p-n junctions.  Transistor: Transfer + Resistor.  It can be either n-p-n type or p-n-p type.  Has three regions with three terminals labeled as i. Emitter (E) ii. Base (B) and iii. Collector (C) The Bipolar Junction Transistor (BJT)
  • 14. The Structure: npn & pnp  Base is made much narrow.  Emitter is heavily doped (p+, n+).  Base is lightly doped (p-, n-).  Collector is lightly doped (p, n).
  • 15. The Structure: npn & pnp  Transistors can be constructed as two diodes that are connected together.
  • 16. Circuit Symbol  The arrow indicates the direction of current flow.  The current flows from collector to emitter in an n-p-n transistor.  The arrow is drawn on the emitter.  The arrow always points towards the n-type. So the emitter is n-type and the transistor is n-p-n type. Layout and Circuit Symbol: n-p-n Transistor
  • 17. Circuit Symbol  The arrow indicates the direction of current flow.  The current flows from emitter to collector in an p-n-p transistor.  The arrow points towards the n- type.  So the base is n-type and transistor is p-n-p type. Layout and Circuit Symbol: p-n-p Transistor
  • 18. Modes of Operation  Based on the bias voltages applied at the two p-n junctions, transistors can operate in three modes: 1. Cut-off (both EB and CB junctions are reversed biased) 2. Saturation (both EB and CB junctions are forward biased) 3. Active mode (EBJ is forward biased and CBJ is reversed biased)  Cut-off and Saturation modes are used in switching operation.  Active mode is used in amplification purposes.
  • 19. Modes of Operation npn bipolar junction transistor pnp bipolar junction transistor
  • 20. Modes of Operation  Both the junctions are reversed biased.  No current can flow through either of the junctions.  So the circuit is open. Cut-off VBC + + - - VBE Ideal model of BJT in cut-off.
  • 21. Modes of Operation  Both the junctions are forward biased.  So the equivalent circuit can be represented by short-circuit between the base, emitter and collector. Saturation: Ideal Model VBC + + - - VBE Ideal model of BJT in saturation.
  • 22. Active Mode Operation EBJ: Forward Biased CBJ: Reverse Biased ◦ Forward bias of EBJ injects electrons from emitter into base (Emitter current). ◦ Most electrons shoot through the base into the collector (Collector current). ◦ Some emitted electrons recombine with holes in p-type base (Base Current)
  • 24. + + + + + + - - - - - - N P N E C B VBE VCB E-Field Electron diffusion Hole diffusion Active Mode Operation
  • 25. + + + + + + - - - - - - N P N E-Field E C B VBE VCB Electron hole recombination Active Mode Operation
  • 26. Collector current T BE V v s C e I i  • The equation above shows that the BJT is indeed a voltage-dependent current source; thus it can be used as an amplifier. Electrons that diffuse across the base to the CBJ junction are swept across the CBJ depletion to the collector because of the higher potential applied to the collector
  • 27. Active Mode Operation Biasing for Active Mode Carriers injected from forward bias junction (from the emitter labeled E) travel through the intermediate layer (BASE, labeled B) and swept into the COLLECTOR, labeled C by the reverse biased voltage. EBJ: Forward Biased CBJ: Reverse Biased
  • 30. DC Output Characteristics IC vs VCE Characteristics of an npn Transistor Active Breakdown Saturation 
  • 32. Bipolar Junction Transistors: Basics + - + - IE IB IC IE = IB + IC ………(KCL) VEC = VEB + VBC ……… (KVL)
  • 33. Current Gain: – α is the fraction of electrons that diffuse across the narrow Base region – 1- α is the fraction of electrons that recombine with holes in the Base region to create base current • The current Gain is expressed in terms of the β (beta) of the transistor (often called hfe by manufacturers). • β (beta) is Temperature and Voltage dependent. • It can vary a lot among transistors (common values for signal BJT: (20 - 200). BJT characteristics            1 ) 1 ( B C E B E C I I I I I I
  • 34. Active Mode: Terminal Currents Current Relationships and Amplification C E B B C E E C E C I I I I I I I I I I       / .                B C B B C I I I I I and 1 1  As  is close to unity,  is very large, typically around 100.   represents the current amplification factor from base to collector.  The base current is amplified by a factor of  in the collector circuit in the Active mode.   is called the Forward Current Gain, often written as  F. C C C B I I I I        1
  • 35.
  • 36. Operation Region IB or VCE Char. BC and BE Junctions Mode Cutoff IB = Very small Reverse & Reverse Open Switch Saturation VCE = Small Forward & Forward Closed Switch Active Linear VCE = Moderate Reverse & Forward Linear Amplifier Break- down VCE = Large Beyond Limits Overload Operation region summary